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A. N. Prokofyev, PNPI 1 Study of inelastic p- and dp- scattering in Roper resonance region A.N.Prokofyev Petersburg Nuclear Physics Institute and SPES4- Collaboration

Study of inelastic a p- and dp- scattering in Roper resonance region

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Study of inelastic a p- and dp- scattering in Roper resonance region. A.N.Prokofyev Petersburg Nuclear Physics Institute and SPES4- p Collaboration. - PowerPoint PPT Presentation

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Page 1: Study of inelastic  a p- and dp- scattering in Roper resonance region

A. N. Prokofyev, PNPI 1

Study of inelastic p- and dp- scattering in Roper resonance region

A.N.Prokofyev

Petersburg Nuclear Physics Institute

and SPES4- Collaboration

Page 2: Study of inelastic  a p- and dp- scattering in Roper resonance region

A. N. Prokofyev, PNPI 2

• Inelastic p- and dp-scattering reactions were studied in the energy region of Roper resonance excitation. Due to the spin and isospin conservation there are only two dominant channels which are open for this reaction: production at the projectile and N* production at the target. A simultaneous registration of the scattered projectile and the secondaries allowed to separate one- and two pions decay of the intermediate state and pick out the 2 channel, which is exclusively connected with the N* baryon intermediate state.

• The shape of the obtained 2 invariant mass spectra was compared with the Oset-Fernandez calculation predictions. It was found that the decay of N* is predominantly going through the spin-isospin scalar state The contribution of the decay through intermediate (N* - N) is small.

• The experiment was carried out at - and d-beams of the Saturne-II accelerator (Saclay). The scattered particles were registered using the SPES4 high resolution spectrometer (projectiles) and wide aperture Forward spectrometer (secondary protons nad pions).

Page 3: Study of inelastic  a p- and dp- scattering in Roper resonance region

A. N. Prokofyev, PNPI 3

Main Feynman diagrams for p->’N* (dp->d’N*) reaction.

E.Oset, P.Fernandez et al.

•a. isobar excitation at projectile.

•b,c. N* excitation at the target.

Page 4: Study of inelastic  a p- and dp- scattering in Roper resonance region

A. N. Prokofyev, PNPI 4

The ’ particle spectra for p-inelastic scattering asa function of energy transferred .

Result of the inclusive measurement at Saturne-II -beam.H.P.Morsch et al., PRL 69 (1992) 1326.

Page 5: Study of inelastic  a p- and dp- scattering in Roper resonance region

A. N. Prokofyev, PNPI 5

SPES4- installation general view(not on scale)

Page 6: Study of inelastic  a p- and dp- scattering in Roper resonance region

A. N. Prokofyev, PNPI 6

Forward spectrometer of SPES4- installation.(not in scale)

• ST – straw tube hodoscopes

• X, Y, U, V – drift chambers

Page 7: Study of inelastic  a p- and dp- scattering in Roper resonance region

A. N. Prokofyev, PNPI 7

Page 8: Study of inelastic  a p- and dp- scattering in Roper resonance region

A. N. Prokofyev, PNPI 8

Spes4-parameters

• SPES4 spectrometer. Nominal acceptance: p/p=5.E-4 This experiment acceptance: p/p=5.E-3

• Forward spectrometer. Angular acceptance: xrad,rad dE/dx resolution – 1 MeV TOF resoluion – 1 nsec Spacial resolution – 0.15 mm p/p ~ 0.03 Missing mass resolution – 20 MeV/c2 Accepted momentum region 0.2 – 1.2 GeV/c

Page 9: Study of inelastic  a p- and dp- scattering in Roper resonance region

A. N. Prokofyev, PNPI 9

Reaction p

• Four accepted momentum intervals in comparison with the scale of previous inclusive measurement made by H.P.Morsch.

Page 10: Study of inelastic  a p- and dp- scattering in Roper resonance region

A. N. Prokofyev, PNPI 10

p-reaction

• Missing mass squared spectra for 4 accepted momentum intervals:

• A) secondary protons detected

• B) secondary pions detected

Page 11: Study of inelastic  a p- and dp- scattering in Roper resonance region

A. N. Prokofyev, PNPI 11

Page 12: Study of inelastic  a p- and dp- scattering in Roper resonance region

A. N. Prokofyev, PNPI 12

p-reactionManley approach for two-pions decay of Roper resonance

from: E.Hernandez et al.,PRC 65 (2002) 65201

• Feinman diagrams for two main processes contributing to Roper resonance decay into two pions in Manley approach: Diagram amplitude is proportional to (k1.k2).

• a) – intermediate state.

• b) N() – intermediate state

Page 13: Study of inelastic  a p- and dp- scattering in Roper resonance region

A. N. Prokofyev, PNPI 13

p-reactionManley approach for two-pions decay of Roper resonance

from: E.Hernandez et al., PRC (2002) 65201

Page 14: Study of inelastic  a p- and dp- scattering in Roper resonance region

A. N. Prokofyev, PNPI 14

p-reactionComparison with Oset-Fernandez predictions

A=(1+c(k1 . k2) )

Form factor and acceptance are included

Page 15: Study of inelastic  a p- and dp- scattering in Roper resonance region

A. N. Prokofyev, PNPI 15

dp-reaction

Page 16: Study of inelastic  a p- and dp- scattering in Roper resonance region

A. N. Prokofyev, PNPI 16

dp-reaction

Page 17: Study of inelastic  a p- and dp- scattering in Roper resonance region

A. N. Prokofyev, PNPI 17

SUMMARY• The p and dp inelastic scattering reactions were exclusively

studied in the energy transfer region corresponded to the Roper resonance excitation region.

• The registration of the scattered projectiles, as well as the charged secondaries allowed to separate different final states, connected with one and two pions production.

• The data in a region, where the Roper resonance production was expected, demonstrate the dominance of the two pion decay of the intermediate N* state . This can be interpreted as the N* (1440 MeV) baryon production. The next possible baryon state D13(1520 Mev) does not fit the data.

• The comparison of the invariant M mass spectra with the theory predictions demonstrates the dominance of the N* decay through the spin, isospin scalar state The contribution of the decay through the Delta resonance is small. This result is in agreement with the data obtained in pp inelastic scattering study at Uppsala.